Resonating valence bond wavefunctions and classical interacting dimer models
arXiv:1112.4917 · doi:10.1103/PhysRevLett.108.247216
Abstract
We relate properties of nearest-neighbour resonating valence bond (nnRVB) wavefunctions for spin systems on two dimensional bipartite lattices to those of fully-packed classical dimer models with potential energy on the same lattice. We define a cluster expansion of in terms of -body potentials , which are recursively determined from the nnRVB wavefunction on {\em finite subgraphs} of the original lattice. The magnitude of the -body interaction () is of order for small , while reduces to a constant due to the fully-packed nature of the model. At leading non-trivial order on the square lattice, the interacting dimer model only has two-body interactions that favour two parallel dimers on elementary plaquettes. Setting and using the results of earlier work on this interacting dimer model, we find that the long-distance behaviour of the bond-energy correlation function is dominated by an oscillatory term that decays as with for SU(2) spins. This result is in remarkable quantitative agreement with earlier direct numerical studies of the corresponding wavefunction, which give .
4+ pages, 2-column format, 1 figure
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